Electrodynamics of Continuous MediaCovers the theory of electromagnetic fields in matter, and the theory of the macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. The chapters on ferromagnetism and antiferromagnetism and on magnetohydrodynamics have been substantially enlarged and eight other chapters have additional sections. |
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Page 262
... equations ( 76.4 ) in the form Hμax " = 0 . ( 76.6 ) Having elucidated that the quantities E , D , H , B form four ... Maxwell's equations ( 76.2 ) and ( 76.4 ) , form the basis for the electrodynamics of dielectrics in motion . The ...
... equations ( 76.4 ) in the form Hμax " = 0 . ( 76.6 ) Having elucidated that the quantities E , D , H , B form four ... Maxwell's equations ( 76.2 ) and ( 76.4 ) , form the basis for the electrodynamics of dielectrics in motion . The ...
Page 359
... Maxwell's equations in the form 1 ав curl E = - - div B = 0 , c at curl B = 1 JD c at div D = 0 , ( 103.3 ) ( 103.4 ) without using H in addition to the mean magnetic field h = B. Instead , all terms which result from averaging the ...
... Maxwell's equations in the form 1 ав curl E = - - div B = 0 , c at curl B = 1 JD c at div D = 0 , ( 103.3 ) ( 103.4 ) without using H in addition to the mean magnetic field h = B. Instead , all terms which result from averaging the ...
Page 385
... Equations for them are obtained by multiplying equation ( 109.5 ) by e , and by e2 . Since waves with E。= constant are exact solutions of Maxwell's equations in the linear approximation , the linear terms in these equations that do not ...
... Equations for them are obtained by multiplying equation ( 109.5 ) by e , and by e2 . Since waves with E。= constant are exact solutions of Maxwell's equations in the linear approximation , the linear terms in these equations that do not ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
Copyright | |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ electric field electromagnetic electrons ellipsoid expression external field factor ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation satisfied scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ